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Abstract

Monodispersed magnetite (Fe3O4) particles were synthesized using a high-temperature hydrolysis reaction with the
assistance of ethylenediaminetetraacetic acid (EDTA) as capping ligands. These particles
were composed of small primary nanocrystals and their sizes could be tuned from about
400 to about 800 nm by simply changing the EDTA or precursor concentration. Surface-tethered
EDTA made the particles highly water-dispersible. The as-prepared magnetite particles
also showed superparamagnetic behavior at room temperature, and their magnetic properties
were size dependent. In addition, the particles had a strong response to external
magnetic field due to their high magnetization saturation values. These properties
were very important for some potential biomedical applications, such as magnetic separation
and magnetic-targeted substrate delivery.

Keywords:

Magnetite; Magnetic properties; Nanocrystalline materials

Background

Over the past decade, magnetic nanocrystals (e.g., Fe3O4, γ-Fe2O3) have attracted much attention due to their unique magnetic properties and important
applications such as targeted drug delivery [1,2], biomolecular separations [3,4], treatment of hyperthermia in cancer [5,6], and as contrast agents in magnetic resonance imaging (MRI) [7,8]. Up to now, many methods have been developed to prepare Fe3O4 nanocrystals with small sizes on the nanometer scale, which include hydrothermal
synthesis [9,10], chemical coprecipitation [11-13], and thermal decomposition and/or reduction [14,15]. Besides these nanosized particles, the secondary structural superparamagnetic Fe3O4 particles have also attracted increasing attention due to their practical applications
in magnetic separation and magnetic-targeted substrate delivery [16,17]. Generally, these secondary structural Fe3O4 particles consist of small Fe3O4 nanocrystals. As-prepared Fe3O4 particles are stable in solution and reveal rapid magnetic response to the externally
applied magnetic field. Over the past decade, these secondary structural Fe3O4 particles are prepared by a common two-step process, including cooperative assembly
[18], microemulsion templating [19], and spontaneous assembly [20]. Compared to the two-step process of assembling the pre-synthesized Fe3O4 nanocrystals into uniform secondary structures, the direct one-step growth route
to synthesize the secondary structural Fe3O4 particles seems to be a simpler way, which is also economical for large-scale production.

Herein we reported a general approach for the fabrication of monodispersed, highly
water-dispersible, and superparamagnetic Fe3O4 particles by a one-step hydrothermal procedure using an ethylenediaminetetraacetic
acid (EDTA)-assisted route. Biocompatible EDTA was chosen because it can act as a
crystal grain growth inhibitor for the synthesis of variously sized Fe3O4 particles, and the carboxylate groups of EDTA have a strong coordination affinity
to the iron cations on the Fe3O4 surface, which might favor the attachment of hydrophilic groups on the surface of
the Fe3O4 particles. Herein, the Fe3O4 particles synthesized with the assistance of EDTA were also intrinsically stabilized
with a layer of hydrophilic ligand in situ, which was essential for their long-term stability in aqueous media without any surface
modification.

Methods

Synthesis of Fe3O4 particles

In a typical synthesis of 725 nm Fe3O4 particles, 1.3 g of anhydrous FeCl3 was first vigorously mixed with 40 mL of ethylene glycol (EG) to form a clear solution.
Then, 0.47 g of EDTA was added and the mixture was heated at 110°C, followed by dissolving
of anhydrous sodium acetate (NaOAc) (2.4 g), Then the mixture was transferred into
a 100-mL Teflon-lined stainless-steel autoclave and sealed in air. The autoclave was
kept at 200°C for 10 h. The black products were collected by a magnet and washed with
ethanol three times, and the products were dried at 60°C for further use.

Characterizations

The x-ray diffraction (XRD) patterns were collected between 20° and 80° (2θ) on an x-ray diffraction system (X’Pert Pro, PANalytical Co., Almelo, The Netherlands)
with a graphite monochromator and Cu Kα radiation (λ = 0.15406 nm). Transmission electron microscope (TEM) images and selected area electron
diffraction (SAED) patterns were obtained (JEOL JEM-2100; JEOL, Tokyo, Japan) operated
at an accelerating voltage of 200 kV. The samples for TEM and high-resolution transmission
electron microscope (HR-TEM) analyses were prepared by spreading a drop of as-prepared
magnetite nanoparticle-diluted dispersion on copper grids coated with a carbon film
followed by evaporation under ambient conditions. Atom force microscope (AFM) characterization
was carried out using Scan Asyst-Air (Bruker Multimode 8, Bruker Corporation, Billerica,
MA, USA). Measurements were carried out in air, and imaging was performed in tapping
mode. The height, amplitude, and phase images were recorded. The scanning electron
microscopy (SEM) images were obtained using LEO 1530 microscope (LEO, Munich, Germany).

Results and discussion

The morphology of the as-prepared Fe3O4 particles was characterized by SEM (Figure 1). As shown in Figure 1A, when FeCl3 concentration is low (0.05 mol L−1), the products are nonuniform, consisting of spherical nanocrystal clusters and small
nanocrystal aggregations. However, when the FeCl3 concentration is in the range of 0.10 to 0.20 mol L−1, all of Fe3O4 particles have a nearly spherical shape (Figure 1B,C). The diameters of the particles slightly increase from 622 ± 145 nm to 717 ± 43
nm, but their sizes become more uniform with the increase of FeCl3 concentration, indicating that higher FeCl3 concentrations could lead to a larger and more uniform particle size.

The surface morphology of the as-obtained Fe3O4 particles is further shown in Figure 2. The 2D and 3D AFM images of Fe3O4 particles prepared from 0.20 mol L−1 of FeCl3 appear a nearly uniform size of about 725 nm and spherical shape, which is in good
agreement to the SEM results (Figure 1C). Furthermore, a high-resolution AFM image of an isolated Fe3O4 particle (Figure 2B) also indicates that the as-prepared Fe3O4 particles are composed of small nanocrystals with the size of about 7 to 15 nm.

TEM image of the as-prepared Fe3O4 particles (Figure 3A) further demonstrates their uniform sizes and morphology. The secondary structure
of Fe3O4 particles also could be observed more clearly in Figure 3B for the isolated cluster, indicating that the obtained Fe3O4 particles are compact clusters. The HR-TEM image recorded at the edge of the Fe3O4 particles is shown in Figure 3C. Measuring the distance between two adjacent planes in a specific direction gives
a value of 0.30 nm, corresponding to the lattice spacing of (220) planes of cubic
magnetite [21,22]. The SAED pattern (Figure 3D) shows polycrystalline-like diffraction, suggesting that the as-prepared Fe3O4 particles consist of magnetite nanocrystals.

The effects of EDTA concentration on the particle sizes and grain sizes of Fe3O4 particles are further investigated. Without addition of EDTA, the resultant products
have a heterogeneous size distribution and their shapes are nonuniform (Figure 4A,F). When the initial EDTA concentration is increased from 10 to 40 mmol L−1, the sizes of Fe3O4 particles decrease slightly from 794 ± 103 nm to 717 ± 43 nm (Figure 4B,C,D and 4G,H,I) and their size distribution becomes more uniform. However, when the EDTA concentration
further increases to 80 mmol L−1, their sizes decrease significantly to 409 ± 70 nm while their size distribution
becomes heterogeneous again (Figure 4E,J), indicating that higher EDTA concentration favors the formation of Fe3O4 particles with larger size; their size distribution, however, is EDTA concentration
dependent.

To confirm the effects of EDTA concentration on the grain sizes and the corresponding
crystalline structures and phase composition of the as-prepared Fe3O4 particles, the samples obtained with different EDTA concentrations are characterized
by XRD. As shown in Figure 5, all the diffraction peaks are indexed to the spinel structure, known for the Fe3O4 crystal (JCPDS no. 00-003-0863) and no other peaks are detected, indicating that
the products are pure phase Fe3O4. In addition, as the EDTA concentration increases, the broadening in the diffraction
peaks becomes more pronounced. The grain sizes of the Fe3O4 particles calculated from the breadth of the (311) reflection using Debye-Scherrer’s
formula [23,24] decrease dramatically from 14.8 to 7.6 nm when the initial EDTA concentration increases
from 0 to 80 mmol L−1. It is thus concluded that EDTA could act as a stabilizer, which might significantly
suppress the grain growth of the as-synthesized Fe3O4 particles.

As a consequence, a probable mechanism which leads to the resulting Fe3O4 particles with tunable grain size and particle size is proposed as follows (Figure 6). When EDTA is introduced to the FeCl3/EG solution, a significant amount of Fe-EDTA complex is formed. NaOAc is then added
and utilized as an alkali source. In the presence of EG and EDTA, Fe3O4 crystallites are formed first under alkaline condition, followed by further growth
into Fe3O4 nanoparticles as the prolonging of reaction time in this system. The primary Fe3O4 nanoparticles then gradually aggregate into large particles to minimize the surface
energy. In addition, because of the strong coordination between Fe(III) ions and carboxylate
on the surface of particles [9,14,25], the as-prepared Fe3O4 particles also possess a coating of carboxylate and could be easily dispersed in
water (inset in Figure 7). When a magnet is applied, the particles could be completely separated from the
solution within seconds. Once the magnet is withdrawn, the particles could be redispersed
into the water immediately by slight shaking. Furthermore, by increasing the amount
of EDTA, more carboxylate groups could bind to the surface of Fe3O4 particles through the strong coordinating ligand. This results in a decrease of the
size of Fe3O4 grains and particles. Magnetic properties (M-H curves) of Fe3O4 particles synthesized with EDTA over the concentration range of 0 to 40 mmol L−1 are shown in Figure 7. It is obvious that all the Fe3O4 particles have no remanence or coercivity at 300 K and their magnetic properties
are strongly dependent on the sizes of Fe3O4 particles prepared. When the initial EDTA concentration is increased from 10 to 40
mmol L−1, the sizes of Fe3O4 particles slightly decrease from 794 ± 103 nm to 717 ± 43 nm. Their magnetization
saturation (Ms) values simultaneously suffer a corresponding decrease from 74.9 to
48.0 emu g−1. This result also suggests that lower EDTA concentration favors the formation of
Fe3O4 particles with better crystallinity, which is in good agreement to the XRD results.

Figure 6.Schematic representation of the formation of Fe3O4 particles with tunable grain size and particle size.

Figure 7.Hysteresis loops of the Fe3O4 particles obtained with EDTA concentrations. Inset was the photographs of an aqueous solution of Fe3O4 particles without magnetic field and with the externally applied magnetic field.

Conclusions

In summary, a modified solvothermal approach was used to synthesize monodispersed
Fe3O4 particles with the assistance of EDTA, which are composed of numerous primary Fe3O4 nanocrystals with sizes of 7 to 15 nm. Their sizes could be easily tuned over a wide
range of 400 to 800 nm by simply varying the concentration of FeCl3 or EDTA. More importantly, owing to the presence of the carboxylate groups attached
on the surface, the Fe3O4 particles have excellent water dispersibility and dispersing stability. In addition,
the growth mechanism of the secondary structural Fe3O4 particles is discussed. The magnetite particles are also superparamagnetic at room
temperature and have a high magnetization, which enhance their response to external
magnetic field and therefore should greatly facilitate the manipulation of the particles
in practical uses.

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

YY, YZ, and MJ performed the experiments. YW, LS, and YH were involved in experimental
planning and analysis of the results. ZH and GZ designed and planned the experiment
and LS also drafted the manuscript. All authors read and approved the final manuscript.

Acknowledgements

This work was supported by the Natural Science Foundation of China (grant nos. 31271071
and 81072472) and the Natural Science Foundation of Fujian Province (grant no. 2012
J01416) and The Medical Science and Technology Innovation Project of Nanjing Military
Command (10MA078, 2010).